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Journal of the Optical Society of America B

Journal of the Optical Society of America B

| OPTICAL PHYSICS

  • Editor: G. I. Stegeman
  • Vol. 23, Iss. 10 — Oct. 1, 2006
  • pp: 2217–2222

Two-dimensional phase resolution of frequency-resolved optical gating across the midinfrared

S. D. McGrane, R. J. Scharff, and J. Barber  »View Author Affiliations


JOSA B, Vol. 23, Issue 10, pp. 2217-2222 (2006)
http://dx.doi.org/10.1364/JOSAB.23.002217


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Abstract

Spectrally and temporally heterodyned four-wave mixing (FWM) signals in silver thiogallate are reported over a wavelength range of 3 10 μ m . We (1) expose the usefulness of the strong nonresonant FWM in optimizing an apparatus for heterodyned 2D infrared experiments and (2) use heterodyning to measure the 2D phase of a frequency-resolved optical gating (FROG) signal. We report the phase of the 2D FROG signal, as opposed to the 1D phase of the excitation pulses routinely determined from conventional FROG analysis. The 2D FROG phase complements the 2D FROG magnitude in providing intuitive visual analysis of the spectral and temporal phases of femtosecond pulses.

© 2006 Optical Society of America

OCIS Codes
(300.6290) Spectroscopy : Spectroscopy, four-wave mixing
(300.6310) Spectroscopy : Spectroscopy, heterodyne
(320.7100) Ultrafast optics : Ultrafast measurements
(320.7150) Ultrafast optics : Ultrafast spectroscopy

ToC Category:
Ultrafast Optics

History
Original Manuscript: February 7, 2006
Revised Manuscript: June 20, 2006
Manuscript Accepted: June 24, 2006

Citation
S. D. McGrane, R. J. Scharff, and J. Barber, "Two-dimensional phase resolution of frequency-resolved optical gating across the midinfrared," J. Opt. Soc. Am. B 23, 2217-2222 (2006)
http://www.opticsinfobase.org/josab/abstract.cfm?URI=josab-23-10-2217


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  39. Fit coefficients of retrieved spectral phase at 3, 5, and 8 μm (−9.31×10−11 rad/nm 4+1.11×10−6 rad/nm 3−4.93×10−3 rad/nm 2+9.78 rad/nm −7.27×103; 3×10−9 rad/nm3−5×10−5 rad/nm2+0.237 rad/nm−397.33; −4.01×10−19 rad/nm 6+2.07×10−14 rad/nm 5−4.44×10−10 rad/nm 4+5.06×10−6 rad/nm 3−3.24×10− 2+1.10×102 rad/nm −1.56×105).

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